Hg^2＋ -牛血清白蛋白复合体系中蛋白质微观结构的研究

研究了Hg2+在生物体内与牛血清白蛋白相互作用的毒性机理以及蛋白质的微观结构变化.测定了Hg2+与牛血清白蛋白(BSA)复合体系的红外光谱(FT-IR)和圆二色谱(CD),并对图谱进行拟合解析处理.红外光谱实验数据表明Hg2+与BSA发生作用的结合位点可能包括-SH、-OH和-NH基团,采用红外拟合技术对BSA二级结构的变化进行了研究,结果表明蛋白质α-螺旋结构含量降低,β-折叠结构含量升高.圆二色谱图也表明由于一定浓度的Hg2+与BSA结合,从而导致蛋白质的二级结构被破坏,这与拟合红外光谱得到的蛋白质二级结构数据相吻合.Hg2+与牛血清蛋白作用致使蛋白质的构象改变,形成金属离子与蛋白质作用的复合物,因而蛋白质失去活性导致生物体发生病变.     

Pb~(2+)-牛血清白蛋白复合体系中蛋白质二级结构的研究

采用紫外光谱、红外光谱和圆二色谱法研究了Pb2+与牛血清白蛋白(BSA)之间的相互作用和蛋白质微观结构的变化。紫外光谱表明,Pb2+与BSA肽链上的CO存在相互作用,并使蛋白质疏水结构的微环境发生变化;红外光谱研究表明,Pb2+与BSA结合位点可能为—OH和—NH基团,利用二阶导、退卷积和谱线拟合技术对蛋白质红外谱图的酰胺Ⅰ带进行处理推测蛋白质二级结构的变化,结果表明蛋白质α螺旋和β折叠二级结构含量降低,β转角二级结构含量增加;圆二色谱(CD)也表明Pb2+与BSA的结合使蛋白质的构象发生了改变。     

不同水团簇结构Zn（NO3）2稀溶液对BSA构象的影响

研究了Zn(NO3)2稀溶液冷冻-解冻处理前后水团簇结构的变化和对牛血清白蛋白(BSA)构象的影响。Zn(NO3)2稀溶液经冷冻-解冻处理后,由于小的水分子团簇结构的形成,溶液电导率明显增加,密度降低,粘度增加。采用激光显微共聚焦拉曼光谱、傅立叶红外光谱和圆二色光谱研究了与冷冻-解冻处理前后Zn(NO3)2稀溶液作用后BSA构象的变化,结果表明:Zn2+对BSA酰胺Ⅰ带的影响较大,可以降低BSA的α-螺旋结构比例,使BSA的二硫键构象、酪氨酸和色氨酸外环境发生变化。Zn(NO3)2稀溶液经冷冻-解冻处理后,对BSA构象的影响变弱。表现为BSA酰胺Ⅰ带α-螺旋结构含量降低相对较少,对酪氨酸外环境的影响减弱。由此可见冷冻-解冻处理可改变Zn(NO3)2稀溶液水分子的团簇结构,使得溶液的物理化学性质发生变化,进而削弱其对BSA构象的影响。     

含磷三足体稀土铕(Ⅲ)配合物与牛血清白蛋白的作用机理

在pH=7.3的Tris-HCl缓冲溶液(模拟生理条件)中, 采用荧光光谱、 循环伏安曲线和紫外光谱研究了N-二(苯-二氨基甲酰基)甲基磷酸铕(Ⅲ)配合物[Eu(pic)₃L]与牛血清白蛋白(BSA)的相互作用. 实验结果表明: 配合物与BSA可以形成1∶1结合型无荧光复合物Eu(pic)₃L-BSA, Eu(pic)₃L对 BSA 内源荧光的猝灭类型为静态猝灭. 根据双对数回归方程计算出二者在不同温度下的结合常数K及结合位点数n, 通过热力学参数得出配合物与 BSA 之间以氢键和范德华力为主. 根据Foster的偶极-偶极无辐射能量转移机理可知配合物与BSA之间可能以偶极-偶极无辐射能量转移方式进行能量传递. 分别考察了Fe³⁺和Cu²⁺对配合物与BSA结合作用的影响, 推测Fe³⁺和Cu²⁺可能在配合物与BSA间起“离子架桥”作用, 使Eu(pic)₃L-BSA复合物的稳定性增强. 循环伏安法研究结果表明配合物与BSA相互作用形成无电活性的Eu(pic)₃L-BSA复合物, 使得溶液中游离的配合物浓度降低.     

聚(2-甲氧基-5-丁氧基)对苯乙炔/Eu2O3纳米复合材料的合成及其光学效应

采用原位脱氯化氢缩合聚合法制备了聚(2-甲氧基-5-丁氧基)对苯乙炔/氧化铕(PMOBOPV/Eu2O3)纳米复合材料. 傅里叶变换红外(FT-IR)光谱证实了在Eu2O3表面的包覆层为PMOBOPV. 高分辨透射电子显微镜(HRTEM)观察发现, PMOBOPV/Eu2O3纳米复合材料具有核-壳结构, 直径为75-145 nm, 其中PMOBOPV包覆层厚度约为25 nm. 紫外-可见(UV-Vis)吸收光谱表明, 随着Eu2O3含量增加, PMOBOPV/Eu2O3的最大吸收峰发生红移且强度提高. 荧光光谱研究表明, 随着Eu2O3含量增加, PMOBOPV/Eu2O3的最大发射波长发生蓝移且强度提高, Eu2O3与PMOBOPV之间形成了光致电子转移体系, 使π电子离域程度增加, 并且导致荧光量子效率提高. 根据光学禁带宽度(Eg)与入射光子能量(hυ)的关系, 拟合了PMOBOPV/Eu2O3薄膜的光学禁带宽度, 发现随着Eu2O3含量增加, Eg逐步减小. 采用简并四波混频方法测试它们的三阶非线性极化率(χ(3)), 发现随着Eu2O3含量增加, PMOBOPV/Eu2O3纳米复合体的非线性光学响应逐渐增强, 这说明PMOBOPV与Eu2O3之间形成了分子间光致电子转移体系, 产生了复杂的分子间离域π电子非线性运动.     

Cr(Ⅵ)与牛血清白蛋白的相互作用

采用荧光光谱、紫外光谱、CD光谱法研究了K2Cr2O7与牛血清白蛋白(BSA)的相互作用。实验结果表明,铬(Ⅵ)使BSA的紫外吸收降低,峰位红移,表明铬(Ⅵ)与BSA发生较强的相互作用;铬(Ⅵ)酸根离子与BSA形成基态复合物导致BSA内源荧光猝灭,猝灭机理主要为静态猝灭。测定了不同温度下该反应的热力学参数,ΔGθ0,ΔHθ和ΔSθ分别为-12.60kJ/mol和56.60J/(mol.k),表明上述作用过程是一个熵增加、自由能降低的自发分子间作用过程,铬(Ⅵ)酸根离子与BSA之间以静电作用力为主;非辐射能量转移机理确定了铬(Ⅵ)与牛血清白蛋白中色氨酸残基之间的距离r=2.85nm;同步荧光和CD光谱研究表明,铬(Ⅵ)使BSA的二级结构发生改变,α-螺旋含量降低,色氨酸残基所处微环境的极性减小。     

光谱法结合分子对接研究萘酰亚胺衍生物与牛血清白蛋白的相互作用

通过多种光谱方法并结合分子对接研究了萘酰亚胺衍生物(XYFS)与牛血清白蛋白(BSA)之间的相互作用。测试了体系在不同温度下的荧光和吸收光谱,以及时间分辨荧光光谱,发现两者之间主要通过静电作用相互结合,XYFS对BSA的荧光猝灭为静态猝灭。进一步研究了体系的同步荧光光谱和圆二色光谱,随着体系中XYFS浓度的逐渐增大,BSA构象发生了明显变化,其疏水性氨基酸残基逐渐裸露,且BSA的α-螺旋含量增加。分子对接模拟表明XYFS与BSA在SiteⅠ位结合,XYFS与BSA中的精氨酸残基有静电相互作用力。研究结果有助于深入了解萘酰亚胺衍生物与蛋白质相互作用机理及结合特征。     

含磷三足体稀土铕(Ⅲ)配合物与牛血清白蛋白的作用机理

在p H=7.3的Tris-HCl缓冲溶液(模拟生理条件)中,采用荧光光谱、循环伏安曲线和紫外光谱研究了N-二(苯-二氨基甲酰基)甲基磷酸铕(Ⅲ)配合物[Eu(pic)3L]与牛血清白蛋白(BSA)的相互作用.实验结果表明:配合物与BSA可以形成1∶1结合型无荧光复合物Eu(pic)3L-BSA,Eu(pic)3L对BSA内源荧光的猝灭类型为静态猝灭.根据双对数回归方程计算出二者在不同温度下的结合常数K及结合位点数n,通过热力学参数得出配合物与BSA之间以氢键和范德华力为主.根据Foster的偶极-偶极无辐射能量转移机理可知配合物与BSA之间可能以偶极-偶极无辐射能量转移方式进行能量传递.分别考察了Fe3+和Cu2+对配合物与BSA结合作用的影响,推测Fe3+和Cu2+可能在配合物与BSA间起"离子架桥"作用,使Eu(pic)3L-BSA复合物的稳定性增强.循环伏安法研究结果表明配合物与BSA相互作用形成无电活性的Eu(pic)3L-BSA复合物,使得溶液中游离的配合物浓度降低.     

光谱法研究牛血清白蛋白与磷钼酸的相互作用

运用UV-Vis光谱、荧光光谱、同步荧光光谱、FT-IR光谱等手段,研究了在模拟人体生理条件下,牛血清白蛋白(BSA)与磷钼酸的相互作用。UV-Vis光谱显示,加入磷钼酸后,BSA的紫外吸收降低且吸收峰红移,表明磷钼酸与BSA形成了复合物;荧光猝灭光谱显示磷钼酸对BSA有荧光猝灭作用,且其荧光猝灭机理符合静态机制,磷钼酸与BSA结合的结合常数为:Ks=2.539×104L·mol-1;探针实验表明磷钼酸与BSA在结合位点I发生结合;Fster偶极-偶极非辐射能量转移机理确定了磷钼酸在BSA中与第214位色氨酸残基之间的距离r=1.93nm;FT-IR光谱显示磷钼酸诱导BSA的二级结构发生了变化,α-螺旋含量降低。     

1,4-二甲基-6,8-二甲氧基-9,10-蒽醌的合成及其与牛血清白蛋白和DNA的相互作用

合成了大黄素类蒽醌衍生物1,4-二甲基-6,8-二甲氧基-9,10-蒽醌(1)并应用紫外光谱、荧光光谱、圆二色谱等方法研究了其与牛血清白蛋白(BSA)和小牛胸腺DNA(ct-DNA)的相互作用.荧光光谱结果表明,化合物1与BSA的相互作用主要以静态猝灭方式使BSA的内源性荧光发生猝灭;圆二色谱表明,化合物1通过疏水作用及形成氢键破坏了α-螺旋结构,导致BSA分子中的α-螺旋含量下降.在pH 7.4时固定DNA的浓度,加入化合物1后,紫外光谱的最大吸收峰发生红移且吸光度加大.荧光光谱表明,化合物1与DNA-4S green NC的结合为竞争性抑制,并可使溶液体系荧光猝灭;圆二色谱表明,随着化合物1的加入,DNA碱基间作用能迅速减弱,表明化合物1与DNA之间为嵌插作用.此外,MTT方法的结果表明,化合物1对结肠癌细胞株HCT116增殖有明显的抑制作用.     

Vibrational spectra of 1-methyluracilate complex with silver(I) and theoretical studies of the 1-MeU anion

The FT-Raman and FT-infrared spectra of (1-methyluracilato)silver, [Ag(C(5)H(5)N(2)O(2))] in the solid state have been studied. The complex is a polymer in which one silver ion is linearly bonded to two 1-MeU ligands through the deprotonated N(3) sites and another silver ion is tetrahedrally coordinated to the four 1-MeU ligands through the O2 and O4 carbonyl oxygen atoms. The harmonic vibrational frequencies, infrared intensities and Raman scattering activities of the N(3)-deprotonated 1-methyluracilate anion have been calculated using density functional (B3LYP) and ab initio (HF and MP2) methods with the 6-31G(d,p) and 6-31++G(df,pd) basis sets. The calculated potential energy distribution (PED) for the 1-MeU anion has proved to be of great help in assigning the spectra of the title complex. It can be concluded that the two strong Raman bands at 1263 and 796 cm(-1) are diagnostic for the N3-deprotonation of the 1-methyluracilate ring and complexation with silver ion. The linear N-Ag-N stretching vibrations are assigned to the bands at 448 and 362 cm(-1) (IR) and 453, 362 cm(-1) (Raman). The Ag-O stretching vibrations are assigned to the bands in the range of 280-250 cm(-1).     

亚碘酰苯低聚物的结构与振动光谱18O-同位素效应的理论研究

应用LDA-PWC方法对亚碘酰苯低聚物HO-(PhIO)n-H (n＝1～10)(链末端以羟基结束)共10个模型分子进行了理论研究. 计算结果表明PhIO分子链大致呈“T”形, I—O链的两个I—O键键长非常接近, 同时发现I—O链产生扭转, 整个亚碘酰苯低聚物呈螺旋状结构. 应用B3LYP法得到HO-(PhIO)6-H更为精确的亚碘酰苯低聚物稳定构型, 平均I—O键长为0.2089 nm, 标准偏差为0.0007 nm. 理论计算表明在600～400 cm－1段, PhI18O的吸收峰向低波数方向移动, 与实验观测结果一致. 振动模式分析发现该段吸收峰均涉及氧原子, 18O同位素效应将降低各振动峰值的频率. 峰值移动最大的吸收峰为591/566 cm－1 (16O/18O), 与之对应的理论计算值为590.409/557.788 cm－1 (16O/18O), 属于对称伸缩振动ν(I—O—I). 吸收峰(443/436 cm－1)对应的理论计算值为460.627/439.158 cm－1 (16O/18O), 归属于不对称伸缩振动ν(I—O—I).     

Fourier-transform Raman and infrared spectroscopic analysis of dipyrrinones and mesobilirubins

The Fourier-transform Raman (FT-Raman), infrared (FT-IR), and UV-visible absorption spectra of four dipyrrinones and two mesobilirubins have been investigated in the solid state and in CH2Cl2 solutions. A detailed spectral analysis, assignment and discussion of these spectra are presented. The bands at 1735-1738, 1691-1707 and 1359-1377 cm(-1) which were assigned to the stretching vibrations of the C-O-C and C-O-H and symmetric deformation of C-H bonds, respectively, can act as a marker to distinguish the compounds of this class. The striking differences between the spectra of the compounds suggest that mesobilirubin XIIIalpha is tending to adopt as ridge-tile conformation, rather than linear conformation.     

Infrared absorption of CH3OSO detected with time-resolved Fourier-transform spectroscopy

A step-scan Fourier-transform spectrometer coupled with a multipass absorption cell was employed to detect temporally resolved infrared absorption spectra of CH(3)OSO produced upon irradiation of a flowing gaseous mixture of CH(3)OS(O)Cl in N(2) or CO(2) at 248 nm. Two intense transient features with origins near 1152 and 994 cm(-1) are assigned to syn-CH(3)OSO; the former is attributed to overlapping bands at 1154 ± 3 and 1151 ± 3 cm(-1), assigned to the S=O stretching mixed with CH(3) rocking (ν(8)) and the S=O stretching mixed with CH(3) wagging (ν(9)) modes, respectively, and the latter to the C-O stretching (ν(10)) mode at 994 ± 6 cm(-1). Two weak bands at 2991 ± 6 and 2956 ± 3 cm(-1) are assigned as the CH(3) antisymmetric stretching (ν(2)) and symmetric stretching (ν(3)) modes, respectively. Observed vibrational transition wavenumbers agree satisfactorily with those predicted with quantum-chemical calculations at level B3P86∕aug-cc-pVTZ. Based on rotational parameters predicted at that level, the simulated rotational contours of these bands agree satisfactorily with experimental results. The simulation indicates that the S=O stretching mode of anti-CH(3)OSO near 1164 cm(-1) likely makes a small contribution to the observed band near 1152 cm(-1). A simple kinetic model of self-reaction is employed to account for the decay of CH(3)OSO and yields a second-order rate coefficient k=(4 ± 2)×10(-10) cm(3)molecule(-1)s(-1).     

Vibrational spectra of four alkaline earth cyclo-hexaphosphates

FT-IR and FT-Raman spectra of four alkaline earth (Mg, Ca, Sr and Ba) cyclo-hexaphosphates have been recorded and analysed. FT-Raman spectra of the deuterated analogues of these compounds are used to clear the ambiguity regarding the OH vibrations in the low frequency region. The spectra reveal that the P6O18(6) anion ring in all compounds have independent PO4 tetrahedra present in it. The P-O(P)and P-O(M')(M'-Mg, Ca, Sr and Ba) bonds become stronger as the cation size decreases. The P6O18(6-) anion ring is distorted in the Mg and Ca compounds. In the Sr and Ba compounds, free and hydrogen bonded water molecules of varying strength are present, whereas in Mg and Ca compounds no free water molecules exist. The POP bridge angle of the Mg, Ca and Sr compounds are estimated using the correlations between the POP bridge stretching frequencies and the bridge angle value.     

Anti-Stokes Yb3+ emission--valuable structure information in spectra of rare earth compounds measured with FT-Raman spectrometers

Raman spectroscopy is a powerful and simple method which proved to be very useful in studies of solids. The most widely used Raman spectrometers are FT-Raman instruments with YAG:Nd(3+) laser as an excitation source. However, in the case of samples containing rare earth elements, the quality of FT-Raman spectra is often low due to strong fluorescence effects. We show that, in such cases, anti-Stokes part of the Raman spectra often contains strong, well resolved bands identified as multiphonon-assisted emission bands of Yb(3+) present as an impurity. We show on several examples that analysis of these bands may provide useful structure information, similar to that obtained by "Eu structure probe" method in optical spectroscopy. The Yb(3+) emission can be also measured using standard luminescence detection systems. However, the application of FT-Raman system allows one to obtain good quality spectra in a much cheaper, easier and faster way (in times as short as a few seconds). Moreover, high-sensitivity of FT-Raman spectrometers allows to detect even very small amounts of Yb(3+) impurity.     

Vibrational spectroscopy investigation using ab initio and density functional theory analysis on the structure of 3,4-dimethylbenzaldehyde

The FT-IR and FT-Raman spectra of 3,4-dimethylbenzaldehyde (3,4-DMB) has been recorded in the region 4000-400 and 3500-100 cm(-1), respectively. The optimized geometry, frequency and intensity of the vibrational bands of 3,4-DMB were obtained by the ab initio and DFT levels of theory with complete relaxation in the potential energy surface using 6-311G(d,p) basis set. The harmonic vibrational frequencies were calculated and the scaled values have been compared with experimental FT-IR and FT-Raman spectra. The observed and the calculated frequencies are found to be in good agreement. The experimental spectra also coincide satisfactorily with those of theoretically constructed bar type spectrograms.     

聚苯乙烯包覆Y_2O_3:Eu~(3 )颗粒及表征

采用柠檬酸表面修饰 Y2 O3:Eu3 颗粒 ,苯乙烯乳液聚合的方法 ,制备出核 -壳型的 Y2 O3:Eu3 /聚苯乙烯颗粒 .在 FTIR谱图上 ,羰基伸缩振动峰向低波数位移 ;在 XPS谱图上 ,Y3d5 / 2 的电子结合能向高能方向移动 ,表明柠檬酸和颗粒表面发生键合作用 .说明此过程符合吸附层媒介作用机理 :柠檬酸使颗粒表面变成两亲性 ,从而使苯乙烯可吸附在颗粒表面形成包覆无机核的乳液结构 .EDS谱图表明聚苯乙烯均匀地包覆在颗粒表面     

Nondestructive discrimination of ivories and prediction of their specific gravity by Fourier-transform Raman spectroscopy and chemometrics

Fourier-transform (FF) Raman spectroscopy and chemometrics were used for nondestructive analysis of ivories. The discrimination of five kinds of ivories, two subspecies of African elephant, mammoth, hippopotamus, and sperm whale, was investigated, and a calibration model for predicting their specific gravity was developed. FT-Raman spectra were measured in situ for them and chemometrics analyses were carried out for the 3050-350 cm(-1) region. The five kinds of ivories were clearly discriminated from each other on the scores plots of two or three principal components (PCs) obtained by principal component analysis (PCA). The loadings plot for PC 1 shows that the discrimination relies on the content ratio of organic collagenous protein and inorganic hydroxyapatite of ivories. The loadings plot for PC 2 shows that bands due to the CH3 and CH2 stretching modes of the protein also play a role in the discrimination. Using partial least squares regression (PLSR), we developed a calibration model that predicts the specific gravity of the ivories from the FT-Raman spectra. The correlation coefficient and root mean square error of cross validation (RMSECV) of this model were 0.980 and 0.024, respectively.     

Double perovskite structure: a vibrational and luminescence investigation providing a perspective on crystal field strength

The luminescence spectra of Eu(3+) doped in a series of double perovskite lattices Ba(2)LnMO(6) (Ln = Y, Gd; M = Nb, Ta) have been recorded at room temperature and 10 K. Together with FT-IR and FT-Raman spectra and aided by DFT vibrational energy calculations, assignments have been made for the crystal field levels of the (5)D(J) (J = 0,1) and (7)F(J) (J = 0-2) multiplets. The luminescence spectra are consistent with monoclinic symmetry of these systems. The crystal field parameters from the fitting of the energy level data set of Ba(2)YNbO(6):Eu(3+) enable the crystal field strength to be calculated, and the order of magnitude is Cl(-) < O(2-) < F(-) for the EuX(6)(n-) (n = 6 for halogen, 9 for oxide) moieties. For these systems, an empirical linear relationship between crystal field strength and electronegativity of ligand X has been found. By contrast, the nephelauxetic series from the depression of the Slater parameter F(2) is Cl(-) ≈ O(2-) > F(-) > free ion for these systems.